50 MeV, 100 kW cw Superconducting Electron Linac Superconducting... · 2 •High beam current is...
Transcript of 50 MeV, 100 kW cw Superconducting Electron Linac Superconducting... · 2 •High beam current is...
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Isotope Separator On Line RIB
target 238U
fission products
Ion SourcePost-
accelerator
Radioactive Ion Beam
E-Linace- γ
tantalumconverter
50 MeV, 100 kW cw Superconducting Electron LinacBased on 1.3 GHz , 2K, SRF technology
Scheme of photo-fission production of RIB in ANURIB
Injector to be tested at VECC Salt Lake Campus
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• High beam current is more important than high energy
• Present Target technology : 100 kW power handling capacity
•50 MeV, 100 kW (2 mA) – optimum for RIB production
238U Photo-fission cross-section as a function of γ-ray energy & Bremsstrahlung energy distribution
Fission yield per watt electronpower saturates at ~ 50 MeV
Courtesy SPIRAL-II Electron Option Courtesy SPIRAL-II Electron Option
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Production of Neutron-rich RIB using photo-fission of actinide targets
IRIB = Iγ . Ntarget . σfission . Efficiency Factor
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Layout of 10 MeV Injector being installed in
e-Linac test area at VECC Kolkata
300 kV gun LEBT ICM Output energy 10 MeV
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Injector Cryo Module (ICM) built in collaboration with TRIUMF Canada
Being developed at TRIUMF for both the institutes
4K-2K converter
beam
VECC Injector Cryo-Module at TRIUMF
9-cell Niobium cavity made at Pavac, Canada
VECC ICM waiting for dressed cavity in Nov. 2015
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Beam successfully accelerated in VECC Injector Cryo-Module
Einj MeV 0.3
Iinj ; duty factor mA 0.10 ; 0.5%
Eout MeV 9.89
Input power kW 10.1 (CW)
Eacc MV/m 10.6
Beam accelerated to 9.9 MeV on Oct 28, 2016